Abstract
The Levinson theorem for the one-dimensional Schrödinger equation with both local and the nonlocal symmetric potentials is established by the Sturm-Liouville theorem. The critical case where the Schrödinger equation has a finite zero-energy solution is also analyzed. It is shown that the number n+ (n-) of bound states with even (odd) parity is related to the phase shift η+(0)[η (0)] of the scattering states with the same parity at zero momentum as (equation presented) and (equation presented) The problems on the positive-energy bound states and the physically redundant state related to the nonlocal interaction are also discussed.
Original language | English |
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Pages (from-to) | 1529-1541 |
Number of pages | 13 |
Journal | International Journal of Theoretical Physics |
Volume | 39 |
Issue number | 6 |
DOIs | |
State | Published - Jun 2000 |
Externally published | Yes |